Carati, DanieleUniversité Libre de Bruxelles, Bruxelles, Belgium
Author
Geurts, Bernard J.University of Twente, 7500 AE Enschede, The Netherlands
Author
Abstract
Large-Eddy Simulation (LES) with regular explicit filtering is investigated.The partial reconstruction of the filtered-scale stress is done through the tensordiffusivity model of Leonard: it provides for backscatter along the stretching direction(s), and for global dissipation, both also attributes of the exact filtered-scale stress. The necessary truncations (LES grid and numerical method) are responsible for an effective subgrid-scale stress. The explicit filter width must be chosen in relation to the grid size. A natural mixed model is then the tensor-diffusivity model supplemented by a dynamic Smagorinsky term. This model is reviewed, together with useful connections to other models, and is tested against Direct Numerical Simulation (DNS) of turbulent isotropic decay starting with Re f 90: LES is started from a 2563 DNS truncated to 643 or 483 and Gaussian filtered. Diagnostics in this test include energy decay, enstrophy decay and energy spectra. After an initial transient of the dynamic procedure, the mixed model is found to produce good results. The results are similar to those obtained when using the dynamic Smagorinsky model without explicit filtering. The dynamic mixed model appears as a good compromise between sufficient reconstruction of the filtered-scale stress and modeling of the subgrid-scale stress.
NASA Ames Resaerch Center, Moffet Field, CA 94035, USA
Université Libre de Bruxelles, Bruxelles, BelgiumService de Physique Statistique et Plasmas
University of Twente, 7500 AE Enschede, The NetherlandsFaculty of Mathematical Sciences
Citations
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FWB
Winckelmans, G., Wray, A. A., Jeanmart, H., Carati, D., & Geurts, B. J. (2001). Tensor-diffusivity mixed model : balancing reconstruction and truncation. In Bernard J. Geurts (ed.), Modern Simulation Strategies for Turbulent Flows (p. 344 p.). Kluwer Academic Publishers. https://hdl.handle.net/2078.5/209372